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Sign of the color-hyperfine splitting in charmonium P states as a test of perturbative QCD
The sign of the difference in energy between the center of gravity of the {sup 3}{ital P} levels and the {sup 1}{ital P} level in heavy quarkonium is a test of the {alpha}{sub {ital s}}{sup 2} terms in perturbative QCD with a fixed coupling constant. Whereas this energy difference is zero in the Fer...
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Published in: | Physical review. D, Particles and fields Particles and fields, 1992-05, Vol.45 (9), p.3268-3271 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The sign of the difference in energy between the center of gravity of the {sup 3}{ital P} levels and the {sup 1}{ital P} level in heavy quarkonium is a test of the {alpha}{sub {ital s}}{sup 2} terms in perturbative QCD with a fixed coupling constant. Whereas this energy difference is zero in the Fermi-Breit approximation and greater than zero in a generalized Fermi-Breit approximation with asymptotically free potentials, the energy difference is negative in perturbative QCD calculations to one-loop order with a fixed {alpha}{sub {ital s}}. For potentials which reasonably agree with the spin-averaged data, the absolute magnitude of the splitting is calculated to be about 4 MeV or less in charmonium and 2 MeV or less in bottomonium. Since the energy of the {sup 3}{ital P} center of gravity in charmonium is known, a measurement of the energy of the {sup 1}{ital P} level is needed to discriminate between these different schemes. Although the {sup 1}{ital P} levels in bottomonium will probably be harder to measure, we also present results for bottomonium. |
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ISSN: | 0556-2821 1089-4918 |
DOI: | 10.1103/PhysRevD.45.3268 |